FFECT OF HIGH PRESSURE ON THE STRUCTURAL AND VIBRATIONAL PROPERTIES …€¦ · VIBRATIONAL...
Transcript of FFECT OF HIGH PRESSURE ON THE STRUCTURAL AND VIBRATIONAL PROPERTIES …€¦ · VIBRATIONAL...
PH.D. SCHOOL IN PHYSICS (XXVIII CYCLE), “SAPIENZA” UNIVERSITY OF ROME
EFFECT OF HIGH PRESSURE ON THE STRUCTURAL AND
VIBRATIONAL PROPERTIES OF ORGANIC MOLECULAR CRYSTALS
Ph.D. Thesis Project Candidate: Francesco Capitani Supervisor: Prof. Paolo Postorino
SCIENTIFIC BACKGROUND Molecular crystals (MCs) have considerably different structural, electronic, optical and chemical properties
compared to conventional solids such as covalent or ionic crystals. This is due to the weak interactions
taking place between molecules, like Van der Waals, dipole – dipole or Hydrogen bonds, compared to the
relatively strong interactions between atoms in non-molecular solids. Properties of MCs are also
determined by the subtle interplay between intermolecular and intramolecular interactions. These
features, along with the almost infinite choice of molecules as crystal building blocks, have made MCs
appealing in various fields of the scientific research in the last twenty years [1]. In particular, a very active
field on this topic is that of crystal engineering (or supra-molecular chemistry), and this is quite
straightforward if one consider that the aim of crystal engineering is the design of a MC with the desired
physical and chemical properties given only the molecular structure [1]. Therefore, crystal engineering is
quite a matter of theoretical prediction of possible MC structures based mostly on the interplay between
two main features: close packing [2] and intermolecular interactions. The principle of close packing relies
mainly on geometrical considerations, in other words the most stable thermodynamic phase at ambient
conditions is that reduces voids in the crystal structure[2]. Although this has been verified for a large
number of compounds, the existence of very weak and similar kinds of intermolecular interactions allows a
lot of metastable phases the system can kinetically approach [1,3]. This considerations, together with the
fact that the great majority of MCs are formed by organic molecules (that means tens-hundreds of atoms
per unit cell), are responsible for a really complicated energy landscape of MCs already at ambient
conditions [1,3]. This is reflected by the high polymorphism exhibited by organic MCs [3-5]. Despite this
intricate framework, at ambient conditions theoretical models are reliable (when the atoms in the unit cell
are not more than 100) and experimental works capture well the above mentioned features [1,3].
However, when the system is not at ambient conditions, i.e. high pressure (HP) or low-high temperature,
theoretical prediction of MC structures is no more reliable [3,5]. Therefore, systematic experimental works
at extreme conditions are needed in order to have a better understanding of the physics of these systems
and to provide a more severe test for the developing of more accurate theoretical models.
PROJECT Among organic MCs, those formed by polycyclic aromatic hydrocarbons, i.e. molecules made up by fused
benzene rings, have recently attracted the attention of condensed matter physicists. This is because of the
first discover of a superconducting transition in aromatic MCs of picene (C22H14)[6], coronene (C24H12)
[7], phenanthrene (C14H10) [8] and dibenzopentacene (C30H18) [9], upon doping with alkali metals, alkali
earths or rare earths. This discover has led to the appearance of several scientific works, mostly theoretical
[10-12]. Although the discovery has prompted a huge effort in the scientific community, there is still a
remarkable lack of experimental works as a consequence of the complex synthesis of superconducting
samples which, even when successful, produces samples unstable to air exposure and with very low
superconducting fractions.
For this reason, and considered the importance of a systematic and detailed knowledge of the physical
properties of the undoped samples to gain insight on the superconducting phase, my first Ph.D. year has
been devoted to the study of the vibrational properties of aromatic MCs under HP. Pressure has been
chosen because having experimental data on a wide pressure range is very useful for the development of
theoretical models more reliable than those tested on data collected at ambient pressure. Moreover, since
in superconducting samples doping apparently induces both volume change and charge transfer, the use of
HP on pure samples may allow to disentangle these two effects by singling out the modifications of the
vibrational spectrum induced by volume compression only. In particular, my first study has been focused on
solid picene and has been reported in two publications [13,14]. Using Raman and Infrared Spectroscopy,
Diamond Anvil Cells for the generation of HP and with the help of theoretical calculations performed by the
group of Prof. L.Boeri (Graz University of Technology) has been possible to show that picene, despite a
∼20% compression of the unit cell, does not undergo phase transitions up to 8 GPa, with vibrational modes
displaying a smooth and uniform hardening with pressure[14]. Accordingly, the observed reduction of the
peak frequency of the vibrational modes in the doped samples has been ascribed mainly to a charge
transfer effect [14]. It is worth to notice that the performed theoretical calculations showed a very good
agreement with the measured data, making us confident about the used theoretical model. The good
performance of this experimental/theoretical approach has led us to perform a similar study on solid
phenanthrene, but at the moment data analysis and calculations are in progress.
For the next years, the aim of this Ph.D. project is to complete this spectroscopic study and extend it to
other aromatic MCs, moving the main target from superconductivity to the study of intermolecular
interactions in MCs under HP, following the motivations presented in the previous section (see Scientific
Background). To reach the goal, X-Ray Diffraction (XRD) will be the main tool to probe the structural
properties under HP, together with optical spectroscopy and theoretical calculations. The combination of
these techniques, will allow a detailed exploration of the HP region of the phase diagram of some aromatic
MCs. This means trying to understand how the fundamental interplay between close packing and
intermolecular interactions change as a function of pressure and if this lead to new structural phases. This
study, aimed to provide a better understanding of the fundamental physics inside MCs, can also be useful
in other fields, like applied physics, crystal engineering and chemistry. This is quite clear considering that
physical and chemical properties interesting for technological devices [15, 16] or for designing a MCs with a
specific task (like drug delivery[17] or pollutant sequestration[18]) depends on the fundamental
interactions between the molecules in the crystal.
At the beginning, the study will be focused on aromatic molecules belonging to the same class of picene,
i.e. molecules with fused benzene rings in a zig-zag fashion. Picene has 5 benzene rings, so phenanthrene
and chrysene, respectively 3 and 4 rings, are the first candidates. Limiting the study to a well-defined class
of molecules, with known molecular and crystal structure at ambient conditions [19], will allow to reduce
the degrees of freedom to control (usually very high in MCs) and, therefore, to make it more feasible
achieving the fixed goal. In second instance, the study could be extended to MCs with molecules formed by
the same number of benzene rings, but in a different configuration, or with molecules with the same
configuration but increasing the number of benzene rings.
EXPERIMENTAL The project will be based on the use of several experimental techniques, as well as a collaboration with
Prof. L. Boeri (Graz University of Technology) and Dr. Marc Hӧppner (Max Planck Institute, Stuttgart) for
theoretical calculations. A Raman micro-spectrometer for Raman spectroscopy measurements, as well as
Diamond Anvil Cell for high pressure, will be provided by the High Pressure Spectroscopy group (Prof. P.
Postorino) of the Physics Dept. of this University. XRD and Infrared spectroscopy measurements will be
carried out in international synchrotron facilities, like ESRF (Grenoble, France) or ELETTRA (Trieste, Italy). In
particular, the XRD measurements will be in collaboration with the group of Dr. L. Malavasi of the Physical
chemistry Dept. of the University of Pavia, as well as Infrared measurements will be possible thanks to the
well-established collaboration with the SISSI beamline (Prof. S. Lupi) of the ELETTRA synchrotron.
REFERENCES [1] G.R. Desiraju, J. Am. Chem. Soc. 135, 9952 (2013) – perspective article
[2] A. I. Kitaigorodsky, Molecular crystals and molecules, Academic press (1973)
[3] G. R. Desiraju, Nature Mater. 1, 77–79 (2002)
[4] J. Bernstein et al., Angew. Chem., Int. Ed. 38, 3440 (1999)
[5] S.L. Price, “Predicting crystal structures of organic compounds” Chem. Soc. Rev. (2014)
[6] R. Mitsuhashi et al., Nature 464, 76 (2010)
[7] Y. Kubozono et al., Phys. Chem. Chem. Phys. 13, 16476 (2011)
[8] X.F. Wang et al., Nature Comm. 2, 507 (2011)
[9] Xue, M. et al., Sci. Rep. 2, 389 (2012)
[10] A. Subedi et al., Phys. Rev. B 84, 020508 (2011)
[11] T. Kato et al., Phys. Rev. Lett. 107, 077001 (2011)
[12] T. Kambe, et al., Phys. Rev. B 86, 214507 (2012)
[13] B. Joseph et al., J. Phys.: Condens. Matter 24, 252203 (2012)
[14] F. Capitani et al., Phys. Rev. B 88, 144303 (2013)
[15] C. Dimitrakopoulos et al., Adv. Mater. 14, 99 (2002)
[16] A. Troisi et al., J. Phys. Chem. B 109, 1849 (2005)
[17] S.L. Price, Adv. Drug Delivery Rev. 56, 301 (2004)
[18] D. D’Alessandro, Angew.Chem., Int. Ed. 49, 6058 (2010)
[19] G.R. Desiraju et al., Acta Crystallogr. B 85, 473 (1989)